95AG 95AG IT DECAY (LT 16 MS) 2003DO09 10NDS 201010
95AG H TYP=FUL$AUT=S. K. Basu, G. Mukherjee, A. A. Sonzogni$
95AG2 H CIT=NDS 111, 2555 (2010)$CUT=30-Jun-2009$
95AG C {+95}Ag isomers produced in {+58}Ni({+40}Ca,p2n|g) reaction at 3.94
95AG2C MeV/^A, and separated by GSI on-line mass separator. Measured E|g,
95AG3C I|g, |g|g, |b|g|g coin and lifetimes using an array of 13 Ge crystals
95AG4C (a Cluster of 7 crystals, a Clover of 4 crystals, a single Ge
95AG5C detector and a ^LEPS detector). The positrons were measured with a
95AG6C plastic scintillator.
95AG CL T$Deduced from intensity distribution of |g-ray versus time as
95AG2CL measured in grow-in mode
95AG D CC$ FROM BrIcc v2.2b (20-Jan-2009) 2008Ki07, "Frozen Orbitals" appr.
95AG D
95AG P 2531.41 19 (23/2+) 16 MS LT
95AG N 0.86 9 1
95AG CN NR$From |S (IG+CE) =100 to GS
95AG PN 5
95AG L 0.0 (9/2+) 1.85 MS 34
95AG L 822.63 9 (11/2+)
95AG G 822.6 1 36 8 (M1+E2) 0.0017911
95AGS G KC=0.00157 10$LC=0.000186 9$MC=3.53E-5 16$NC=6.1E-6 3$OC=2.85E-7 22$
95AGS G NC+=6.4E-6 4
95AG CG M$M1+E2 assignment according to shell-model calculations
95AG L 936.52 9 (13/2+)
95AG G 936.5 1 80 9 (E2)
95AGS G CC=0.001244 18$KC=0.001085 16$LC=0.0001300 19$MC=2.46E-5 4$
95AGS G NC=4.25E-6 6$OC=1.95E-7 3$NC+=4.45E-6
95AG CG M$E2 assignment according to shell-model calculations
95AG L 1939.79 14 (15/2+)
95AG G 1003.2 1 70 8 (M1+E2) 0.001148
95AGS G KC=0.00100 7$LC=0.000117 7$MC=2.22E-5 13$NC=3.85E-6 24$OC=1.81E-7 15$
95AGS G NC+=4.03E-6 25
95AG CG M$M1+E2 assignment according to shell-model calculations
95AG G 1117.1 1 40 10 (E2)
95AGS G CC=0.000841 12$KC=0.000734 11$LC=8.67E-5 13$MC=1.642E-5 23$
95AGS G NC=2.84E-6 4$OC=1.322E-7 19$NC+=3.91E-6
95AG CG M$E2 assignment according to shell-model calculations
95AG L 2103.60 17 (17/2-)
95AG G 163.8 1 106 11 (E1) 0.0391
95AGX G K/T=0.0328 5$L/T=0.00393 6$M/T=0.000741 11$N/T=0.0001267 18$
95AGX G O/T=5.42E-6 8
95AGS G KC=0.0341 5$LC=0.00408 6$MC=0.000770 11$NC=0.0001317 19$OC=5.63E-6 8$
95AGS G NC+=0.0001373 20
95AG CG M$expected from shell-model; also, because I|g(163.8) is very similar
95AG2CG to I|g(427.8), transition can only be dipole.
95AG L 2531.41 19 (23/2+) 16 MS LT
95AG G 427.8 1 115 8 (E3) 0.0311
95AGX G K/T=0.0249 4$L/T=0.00423 6$M/T=0.000822 12$N/T=0.0001372 20$
95AGX G O/T=4.33E-6 6
95AGS G KC=0.0257 4$LC=0.00437 7$MC=0.000847 12$NC=0.0001415 20$OC=4.47E-6 7$
95AGS G NC+=0.0001459 21
95AG CG M$expected from shell-model, supported by a reasonable value of
95AG2CG BE3W>0.052